{ "id": "1801.02576", "version": "v1", "published": "2018-01-08T17:30:48.000Z", "updated": "2018-01-08T17:30:48.000Z", "title": "Capability of future linear colliders to discover heavy neutral CP-even and CP-odd Higgs bosons within Type-I 2HDM", "authors": [ "Majid Hashemi", "Gholamhossein Haghighat" ], "comment": "32 pages, 29 figures, 11 tables", "categories": [ "hep-ph" ], "abstract": "In this study, assuming the type-I 2HDM at SM-like scenario, observability of heavy neutral CP-even and CP-odd Higgs bosons $H$ and $A$ at a linear collider operating at $\\sqrt{s}=1$ TeV is investigated through the signal process chain $e^- e^+ \\rightarrow A H \\rightarrow ZHH$ where the $Z$ boson experiences a leptonic ($e^-e^+$ or $\\mu^-\\mu^+$) decay and the $H$ Higgs boson is assumed to decay into a di-photon. This signal process is motivated especially by the clean signature which leptonic and photonic events can provide at colliders, and also by the enhancement due to the charged Higgs-mediated contribution to $H$ di-photon decay at large $\\tan\\beta$ values. Simulation is based on four benchmark points according to which the Higgs mass $m_H$ ($m_A$) varies within the range $150$-$300$ ($200$-$400$) GeV. Energy smearing of jets and photons are performed, and momentum smearing is also applied to leptons. Results indicate that, for all of the assumed benchmark points, the Higgs bosons $H$ and $A$ are observable with measurable masses, and with signals exceeding $5\\sigma$ at integrated luminosities $111$ and $201\\,fb^{-1}$ respectively. Such luminosities are easily accessible to future linear colliders.", "revisions": [ { "version": "v1", "updated": "2018-01-08T17:30:48.000Z" } ], "analyses": { "keywords": [ "cp-odd higgs bosons", "heavy neutral cp-even", "linear collider", "type-i 2hdm", "capability" ], "note": { "typesetting": "TeX", "pages": 32, "language": "en", "license": "arXiv", "status": "editable" } } }